Department of Physics, Keio University, Hiyoshi, Yokohama, Japan.
J Phys Condens Matter. 2012 Jan 18;24(2):024201. doi: 10.1088/0953-8984/24/2/024201. Epub 2011 Dec 15.
We observed a magnetic domain wall (DW) motion induced by the spin-polarized pulsed current in a nanoscale Fe(19)Ni(81) wire using a magnetic force microscope. High current density, which is of the order of 10(11) A m(-2), was required for the DW motion. A simple method to estimate the temperature of the wire was developed by comparing the wire resistance measured during the DW motion with the temperature dependence of the wire resistance. Using this method, we found the temperature of the wire was proportional to the square of the current density and became just beneath at the threshold Curie temperature. Our experimental data qualitatively support this analytical model that the temperature is proportional to the resistivity, thickness, width of the wire and the square of the current density, and also inversely proportional to the thermal conductivity.
我们使用磁力显微镜观察到了在纳米级 Fe(19)Ni(81) 金属丝中由自旋极化脉冲电流引起的磁畴壁(DW)运动。DW 运动所需的电流密度高达 10(11) A m(-2) 的数量级。我们通过比较 DW 运动期间测量的金属丝电阻与金属丝电阻随温度的变化关系,开发了一种简单的方法来估计金属丝的温度。使用这种方法,我们发现金属丝的温度与电流密度的平方成正比,并在居里温度阈值以下。我们的实验数据定性地支持了这个分析模型,即温度与电阻率、金属丝的厚度、宽度和电流密度的平方成正比,与热导率成反比。